{"title":"Héterogénéité de la chlorophylle in vivo","authors":"Jean Lavorel","doi":"10.1016/0926-6577(64)90151-2","DOIUrl":null,"url":null,"abstract":"<div><p>A former study of chlorophyll fluorescence in Chlorella had lead to the distinction of several fractions of the chlorophyll holochrome: A photoreceptive fraction Chl<sub>0</sub> and two fractions Chl<sub>1</sub><sup>685</sup> and Chl<sub>1</sub><sup>720</sup> the excition of which was sensitized by the first one. The Chl<sub>1</sub><sup>685</sup> fraction has a potochemical function and is responsible for the variable yield emission. The constant yield emission maily comes from Chl<sub>0</sub> and to a lesser extent from Chl<sub>1</sub><sup>720</sup>.</p><p>By studies of fluorescence polarisation, this scheme of excitation transfers is confirmed; moreover, the Chl<sub>1</sub><sup>720</sup> fraction has a certain amount of direct absorption and a high degree of orientation.</p><p>The variation of fluorescence yield during the induction period is seen as resulting from the distribution of the Chl<sub>1</sub><sup>685</sup> fraction between at least two forms: the non-fluorescent O form and the fluorescent P form. Action spectra of the Chl<sub>1</sub><sup>685</sup> show in the far red a difference between the photochemical production of the P form and the excitation of its fluorescence. This difference can be understood in the theory of two photochemical systems of photosynthesis as resulting from the antagonistic action of each system on the P form.</p><p>The general scheme of electron transport in photosynthesis and the concept of structural separation of the sensitizers of the two systems are discussed.</p></div>","PeriodicalId":100169,"journal":{"name":"Biochimica et Biophysica Acta (BBA) - Specialized Section on Biophysical Subjects","volume":"88 1","pages":"Pages 20-36"},"PeriodicalIF":0.0000,"publicationDate":"1964-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0926-6577(64)90151-2","citationCount":"28","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Biochimica et Biophysica Acta (BBA) - Specialized Section on Biophysical Subjects","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0926657764901512","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 28
Abstract
A former study of chlorophyll fluorescence in Chlorella had lead to the distinction of several fractions of the chlorophyll holochrome: A photoreceptive fraction Chl0 and two fractions Chl1685 and Chl1720 the excition of which was sensitized by the first one. The Chl1685 fraction has a potochemical function and is responsible for the variable yield emission. The constant yield emission maily comes from Chl0 and to a lesser extent from Chl1720.
By studies of fluorescence polarisation, this scheme of excitation transfers is confirmed; moreover, the Chl1720 fraction has a certain amount of direct absorption and a high degree of orientation.
The variation of fluorescence yield during the induction period is seen as resulting from the distribution of the Chl1685 fraction between at least two forms: the non-fluorescent O form and the fluorescent P form. Action spectra of the Chl1685 show in the far red a difference between the photochemical production of the P form and the excitation of its fluorescence. This difference can be understood in the theory of two photochemical systems of photosynthesis as resulting from the antagonistic action of each system on the P form.
The general scheme of electron transport in photosynthesis and the concept of structural separation of the sensitizers of the two systems are discussed.